Using the HST/ACS $I_{\rm F814W}$-band data, we investigated distribution of apparent axial ratios of $\sim21000$ galaxies with $M_{V}<-20$ at $0.2<z<1.0$ in the COSMOS field as a function of stellar mass, specific star formation rate (sSFR), and redshift. We statistically estimated intrinsic 3-dimensional shapes of these galaxies by fitting the axial-ratio distribution with triaxial ellipsoid models characterized by face-on (middle-to-long) and edge-on (short-to-long) axial ratios $B/A$ and $C/A$. We found that the transition from thin disk to thick spheroid occurs at $Δ$MS $\sim-1$ dex, i.e., 10 times lower sSFR than that of the main sequence for galaxies with $M_{\rm star} = 10^{10}$--$10^{11} M_{\odot}$ at $0.2<z<1.0$. Furthermore, the intrinsic thickness ($C/A$) of passively evolving galaxies with $M_{\rm star}=10^{10}$--$10^{11}M_{\odot}$ significantly decreases with time from $C/A \sim 0.40$ -- $0.50$ at $z\sim 0.8$ to $C/A\sim0.33$ -- $0.37$ at $z\sim0.4$, while those galaxies with $M_{\rm star}>10^{11}M_{\odot}$ have $C/A\sim0.5$ irrespective of redshift. On the other hand, star-forming galaxies on the main sequence with $10^{9.5}$--$10^{11}M_{\odot}$ show no significant evolution in their shape at $0.2<z<1.0$, but their thickness depends on stellar mass;more massive star-forming galaxies tend to have lower $C/A$ (thinner shape) than low-mass ones. These results suggest that some fraction of star-forming galaxies with a thin disk, which started to appear around $z\sim1$, quench their star formation without violent morphological change, and these newly added quiescent galaxies with a relatively thin shape cause the significant evolution in the axial-ratio distribution of passively evolving galaxies with $M_{\rm star}<10^{11}M_{\odot}$ at $z<1$.
Dust Heating by Low-mass Stars in Massive Galaxies at z<1
利用Hubble空间望远镜/Wide Field Camera 3的成像数据和多波长光度表,研究了CANDELS场中0.2<z<1.0处被动演化星系和恒星形成星系的尘埃温度。我们从这些星系的恒星质量和表面亮度分布估算了低质量恒星的恒星辐射场,并计算了它们的稳态尘埃温度。首先,我们使用赫歇尔室女星系团巡天的深远红外数据,使用附近的早型星系测试了我们的方法,并证实估计的尘埃温度与观测到的温度在不确定性范围内是一致的。然后我们将该方法应用于0.2<z<1.0的星系,发现大多数Mstar > 10^{10} Msun的被动演化星系都具有较高的尘埃温度(Tdust > 20 K),因此实验室实验预计在弥漫ISM中尘埃颗粒表面分子氢的形成效率很低。被动演化星系的比例强烈依赖于所有红移处的预期尘埃温度,并随着温度的增加而迅速增加。这些结果表明,大质量星系中低质量恒星对尘埃的加热对大质量星系被动演化的继续起着重要作用,因为缺乏氢分子对紫外辐射的屏蔽作用,阻止了气体冷却和新恒星的形成。
HC$_3$N, H$^{13}$CN, and HN$^{13}$C in molecular cores evolving towards star-forming regions
Instituto de Investigaciones en Energía No Convencional, CONICET-UNSa(非常规能源研究所,CONICET-UNSA);Departamento de Física, Facultad de Ciencias Exactas y Naturales, UBA(理学院自然科学系物理系,UBA);Departamento de Matemática, Facultad de Ciencias Exactas, Universidad Nacional de Salta(理学院数学系,萨尔塔国立大学);Instituto de Astronomía y Física del Espacio, CONICET-UBA(天体物理学与空间研究所,CONICET-UBA)
MIGHTEE: The evolving radio luminosity functions of star-forming galaxies to $z\sim 4.5$ and the cosmic history of star formation
University of Oxford(牛津大学);UKRI STFC Rutherford Appleton Laboratory(英国研究与创新部STFC拉瑟福德阿普尔顿实验室);University of the Western Cape(西开普大学);Institute for Astronomy, University of Edinburgh(爱丁堡大学天文研究所);Carnegie Observatories(卡内基观测站);Rhodes University(罗德兹大学)
Radio Continuum Emission from Evolving Star-Forming Galaxies -- I. Correlations Involving the Total Synchrotron Luminosity
National Institute of Science Education and Research(国家科学教育与研究中心);Homi Bhabha National Institute(霍米·巴巴国立研究所);Department of Physics, CUSAT(科钦大学天体物理与空间应用学院物理系);School of Mathematics, Statistics and Physics, Newcastle University(纽卡斯尔大学数学、统计与物理学院);Antonie(安东尼公司);School of Astronomy, Institute for Research in Fundamental Sciences (IPM)(基础科学研究院天体物理学院)
Cosmography via stellar archaeology of low-redshift early-type galaxies from SDSS
Scuola Internazionale Superiore di Studi Avanzati (SISSA)(高等国际研究学校);Institute for Fundamental Physics of the Universe (IFPU)(宇宙基础物理研究所);Universitat Heidelberg(海德堡大学);University of Trento(特伦托大学);IRA-INAF(国家天体物理研究所阿布鲁佐天文台);INFN-Sezione di Trieste(意大利国家核物理研究所的里雅斯特分部)
Forged in Quenching: Morphological Transformation across Star-forming and Quiescent Galaxies in EAGLE
Institute for Computational Cosmology, Department of Physics, Durham University(达勒姆大学物理学院宇宙计算研究所);Centre for Extragalactic Astronomy, Department of Physics, Durham University(达勒姆大学物理学院河外天文学中心);Institute for Data Science, Durham University(达勒姆大学数据科学研究所);Center for Astronomy and Astrophysics and Department of Physics, Fudan University(复旦大学物理学院天文与天体物理中心)
Looking into the faintEst WIth MUSE (LEWIS): Exploring the nature of ultra-diffuse galaxies in the Hydra-I cluster. VI. A star-forming UDG in Hydra I: a rare UDG or a transition phase?
University of Naples “Federico II”(那不勒斯费德里科二世大学);Armagh Observatory and Planetarium(阿马赫天文台和天文馆);Gran Sasso Science Institute(格兰萨索科学研究所);Finnish Centre for Astronomy with ESO, (FINCA), University of Turku(图尔库大学芬兰ESO天文中心);Tuorla Observatory, Department of Physics and Astronomy, University of Turku(图尔库大学物理与天文学系图奥拉天文台);Turku Collegium for Science(图尔库科学学院)
The Nuclear Star Cluster of M 74: a fossil record of the very early stages of a star-forming galaxy
Instituto de Astrofísica de Canarias(加那利天体物理研究所);Universidad de La Laguna(拉古纳大学);Max-Planck-Institut für Astronomie(马克斯·普朗克天文学研究所);Université Côte d’Azur(蔚蓝海岸大学);Observatoire de la Côte d’Azur(蔚蓝海岸天文台)
Star-forming environments in smoothed particle magnetohydrodynamics simulations II: Re-simulating isolated clumps to determine equivalence of extracted clumps and parent simulations
The VLA Survey of the Chandra Deep Field South. V. Evolution and Luminosity Functions of sub-mJy radio sources and the issue of radio emission in radio-quiet AGN
The bending of the star-forming main sequence traces the cold- to hot-accretion transition mass over 0<z<4
我们分析了恒星质量(M0)的变化,在那里恒星形成的主序列(MS)的弯曲发生在0<z<4。我们发现在0<z<1时M0~10^10Msun,然后在z=2时M0上升到~10^11Msun,然后保持平稳或向更高的红移缓慢增加。当转换成托管暗物质晕质量的M0值,我们表明,这种行为是非常一致的不断发展的冷到热吸积过渡质量,理论预测和定义的红移无关的Mshock在z <1.4 and by the rising Mstream at z>1.4(我们提出了一个修订与最新的模拟协议)。因此,我们认为MS弯曲主要是由于冷吸积的减少导致星系中可用冷气体的减少,并支持气体馈送理论的预测。特别是,在z>1处红移的快速上升的M0证实了冷流情景的证据。在这幅图中,在质量大于M0的星系中,逐渐减少燃料而不是突然抑制质量大于Mshock/Mstream的晕,会产生几乎恒定的恒星形成速率,而不是它们的淬灭,因此需要其他物理过程。与星系恒星质量函数中的膝盖M* 相比,M0在z<1.5时显着较低,在z>2时较高,这表明气体匮乏对星系质量分布的影响发生在早期(z>1.5-2)。MS内部星系成为膨胀主导的典型质量与M0的演变不同,这与膨胀形成是一个与冷吸积逐渐消失不同的过程的想法一致。
Molecular gas properties of star-forming brightest group galaxies at $z \sim 0.3$
Alma Mater Studiorum Università di Bologna(博洛尼亚大学);INAF - Osservatorio di Astrofisica e Scienza dello Spazio di Bologna(意大利国家天体物理研究所波伦亚天文台);Zentrum für Astronomie, Universität Heidelberg(海德堡大学天文中心);Observatoire de Paris, Collège de France, PSL University, Sorbonne University, CNRS, LUX(巴黎天文台,法兰西学院,PSL大学,索邦大学,法国国家科学研究中心,LUX);Institut de Radioastronomie Millimétrique (IRAM)(毫米波射电天文研究所);INFN - Sezione di Bologna(意大利国家核物理研究所博洛尼亚分部);ITP, Universität Heidelberg(海德堡大学理论物理研究所)